This repository has been archived on 2023-11-20. You can view files and clone it, but cannot push or open issues or pull requests.
foam-extend4.1-coherent-io/applications/solvers/combustion/PDRFoam/PDRModels/turbulence/PDRkEpsilon/PDRkEpsilon.C

316 lines
7 KiB
C

/*---------------------------------------------------------------------------*\
========= |
\\ / F ield | OpenFOAM: The Open Source CFD Toolbox
\\ / O peration |
\\ / A nd | Copyright held by original author
\\/ M anipulation |
-------------------------------------------------------------------------------
License
This file is part of OpenFOAM.
OpenFOAM is free software; you can redistribute it and/or modify it
under the terms of the GNU General Public License as published by the
Free Software Foundation; either version 2 of the License, or (at your
option) any later version.
OpenFOAM is distributed in the hope that it will be useful, but WITHOUT
ANY WARRANTY; without even the implied warranty of MERCHANTABILITY or
FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public License
for more details.
You should have received a copy of the GNU General Public License
along with OpenFOAM; if not, write to the Free Software Foundation,
Inc., 51 Franklin St, Fifth Floor, Boston, MA 02110-1301 USA
\*---------------------------------------------------------------------------*/
#include "PDRkEpsilon.H"
#include "wallFvPatch.H"
#include "PDRDragModel.H"
#include "addToRunTimeSelectionTable.H"
// * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * //
namespace Foam
{
namespace compressible
{
namespace RASModels
{
// * * * * * * * * * * * * * * Static Data Members * * * * * * * * * * * * * //
defineTypeNameAndDebug(PDRkEpsilon, 0);
addToRunTimeSelectionTable(RASModel, PDRkEpsilon, dictionary);
// * * * * * * * * * * * * * * * * Constructors * * * * * * * * * * * * * * //
PDRkEpsilon::PDRkEpsilon
(
const volScalarField& rho,
const volVectorField& U,
const surfaceScalarField& phi,
basicThermo& thermophysicalModel
)
:
RASModel(typeName, rho, U, phi, thermophysicalModel),
Cmu_
(
dimensioned<scalar>::lookupOrAddToDict
(
"Cmu",
coeffDict_,
0.09
)
),
C1_
(
dimensioned<scalar>::lookupOrAddToDict
(
"C1",
coeffDict_,
1.44
)
),
C2_
(
dimensioned<scalar>::lookupOrAddToDict
(
"C2",
coeffDict_,
1.92
)
),
alphak_
(
dimensioned<scalar>::lookupOrAddToDict
(
"alphak",
coeffDict_,
1.0
)
),
alphaEps_
(
dimensioned<scalar>::lookupOrAddToDict
(
"alphaEps",
coeffDict_,
0.76923
)
),
alphah_
(
dimensioned<scalar>::lookupOrAddToDict
(
"alphah",
coeffDict_,
1.0
)
),
k_
(
IOobject
(
"k",
runTime_.timeName(),
mesh_,
IOobject::MUST_READ,
IOobject::AUTO_WRITE
),
mesh_
),
epsilon_
(
IOobject
(
"epsilon",
runTime_.timeName(),
mesh_,
IOobject::MUST_READ,
IOobject::AUTO_WRITE
),
mesh_
),
mut_
(
IOobject
(
"mut",
runTime_.timeName(),
mesh_,
IOobject::NO_READ,
IOobject::NO_WRITE
),
Cmu_*rho_*sqr(k_)/(epsilon_ + epsilonSmall_)
)
{
# include "wallViscosityI.H"
printCoeffs();
}
// * * * * * * * * * * * * * * * Member Functions * * * * * * * * * * * * * //
tmp<volSymmTensorField> PDRkEpsilon::R() const
{
return tmp<volSymmTensorField>
(
new volSymmTensorField
(
IOobject
(
"R",
runTime_.timeName(),
mesh_,
IOobject::NO_READ,
IOobject::NO_WRITE
),
((2.0/3.0)*I)*k_ - (mut_/rho_)*dev(twoSymm(fvc::grad(U_))),
k_.boundaryField().types()
)
);
}
tmp<volSymmTensorField> PDRkEpsilon::devRhoReff() const
{
return tmp<volSymmTensorField>
(
new volSymmTensorField
(
IOobject
(
"devRhoReff",
runTime_.timeName(),
mesh_,
IOobject::NO_READ,
IOobject::NO_WRITE
),
-muEff()*dev(twoSymm(fvc::grad(U_)))
)
);
}
tmp<fvVectorMatrix> PDRkEpsilon::divDevRhoReff(volVectorField& U) const
{
return
(
- fvm::laplacian(muEff(), U) - fvc::div(muEff()*dev2(fvc::grad(U)().T()))
);
}
bool PDRkEpsilon::read()
{
if (RASModel::read())
{
Cmu_.readIfPresent(coeffDict_);
C1_.readIfPresent(coeffDict_);
C2_.readIfPresent(coeffDict_);
alphak_.readIfPresent(coeffDict_);
alphaEps_.readIfPresent(coeffDict_);
alphah_.readIfPresent(coeffDict_);
return true;
}
else
{
return false;
}
}
void PDRkEpsilon::correct()
{
if (!turbulence_)
{
// Re-calculate viscosity
mut_ = rho_*Cmu_*sqr(k_)/(epsilon_ + epsilonSmall_);
# include "wallViscosityI.H"
return;
}
RASModel::correct();
volScalarField divU = fvc::div(phi_/fvc::interpolate(rho_));
if (mesh_.moving())
{
divU += fvc::div(mesh_.phi());
}
tmp<volTensorField> tgradU = fvc::grad(U_);
volScalarField G = 2*mut_*(tgradU() && dev(symm(tgradU())));
tgradU.clear();
// Add the blockage generation term so that it is included consistently
// in both the k and epsilon equations
const volScalarField& betav = U_.db().lookupObject<volScalarField>("betav");
const PDRDragModel& drag =
U_.db().lookupObject<PDRDragModel>("PDRDragModel");
volScalarField GR = drag.Gk();
# include "wallFunctionsI.H"
// Dissipation equation
tmp<fvScalarMatrix> epsEqn
(
betav*fvm::ddt(rho_, epsilon_)
+ fvm::div(phi_, epsilon_)
- fvm::laplacian(DepsilonEff(), epsilon_)
==
C1_*(betav*G + GR)*epsilon_/k_
- fvm::SuSp(((2.0/3.0)*C1_)*betav*rho_*divU, epsilon_)
- fvm::Sp(C2_*betav*rho_*epsilon_/k_, epsilon_)
);
# include "wallDissipationI.H"
epsEqn().relax();
solve(epsEqn);
bound(epsilon_, epsilon0_);
// Turbulent kinetic energy equation
tmp<fvScalarMatrix> kEqn
(
betav*fvm::ddt(rho_, k_)
+ fvm::div(phi_, k_)
- fvm::laplacian(DkEff(), k_)
==
betav*G + GR
- fvm::SuSp((2.0/3.0)*betav*rho_*divU, k_)
- fvm::Sp(betav*rho_*epsilon_/k_, k_)
);
kEqn().relax();
solve(kEqn);
bound(k_, k0_);
// Re-calculate viscosity
mut_ = rho_*Cmu_*sqr(k_)/epsilon_;
# include "wallViscosityI.H"
}
// * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * //
} // End namespace RASModels
} // End namespace compressible
} // End namespace Foam
// ************************************************************************* //